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Assessment of the Bill Emerson Memorial Bridge - FTP Directory ...

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For a group <strong>of</strong> piles with identical geometry, <strong>the</strong> group interaction factor isa summation <strong>of</strong> those factors from individual piles. Note that <strong>the</strong> group interactionfactor in horizontal x-direction and y-direction may be different, depending on <strong>the</strong>number and <strong>the</strong> spacing <strong>of</strong> piles in each direction.A.3 Group stiffness and damping factorsFigure A.4 shows schematically <strong>the</strong> plan and cross sections <strong>of</strong> an arbitrarypile group foundation. This figure will be used to explain and obtain <strong>the</strong> stiffnessand damping factors <strong>of</strong> a group <strong>of</strong> piles in all directions. For vertical vibration, <strong>the</strong>group stiffness (k g ) and damping factors (c g ) can be expressed intozz∑ k ∑ cc gzk gzz = ,z = (α A∑∑α AFor torsional vibration, <strong>the</strong> group stiffness (k gψ ) and damping factors (c gψ )can be evaluated by= [ k + k ( )]1k g 2 2ψ ψ xx r+ yr∑αA2, c ψ= [cψ+ c x( x r+ y 2∑α Ag 1r)]A.6)(A.7)For translational modes, <strong>the</strong> group stiffness and damping coefficientsalong x axis (kx g, cx g ) and along y axis (ky g, cy g ) can be determined by∑ k ∑ c ∑ c gxk ∑x = k g yck gxy = c g yx = , , ,y = (A.8)∑α Lx ∑α Lx ∑α LA ∑α LyFor rocking vibration about y axis and about x axis, <strong>the</strong> stiffness anddamping coefficients (kφ g, cφ g ) and (kθ g, cθ g ) can be respectively evaluated byk k 2 2g zxrk xz c2z ckk = + + − φ x φc c x 2 2g φ z rc xz c2z cc xφ, c+ + −∑α = φ(A.9)φLx∑α Lx2 2k kg θ zyrk yz c2z ckk+ + − 2 2=yθc + c +g θ zyrc xz c−2z ccθ, c∑α = yθ(A.10)θLy∑α LyFor <strong>the</strong> coupled vibration between translational mode along x axis androtational mode about y axis, <strong>the</strong> group stiffness and damping coefficients (kxφ g,cxφ g ) can be evaluated by1k g = 1xφ ∑ ( k xφ− k xzc), c gαLxxφ = ∑ ( )α Lxc xφ− c xz c(A.11)Similarly, <strong>the</strong> group stiffness and damping coefficients for <strong>the</strong> coupled vibrationbetween translational mode along y axis and rotation al mode about x axis, (kyθ g,cyθ g ), can be expressed into11k g yθ= ∑ ( k yθ− k yzc), c g yθ= ∑ (c yθ− c yzααLyLyc)(A.12)105

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